Oldroyd-B model
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The Oldroyd-B model is a constitutive model used to describe the flow of viscoelastic fluids. This model can be regarded as an extension of the Upper Convected Maxwell model and is equivalent to a fluid filled with elastic bead and spring dumbbells. The model is named after its creator James G. Oldroyd.
The model can be written as:
where:
- is the stress tensor;
- is the relaxation time;
- is the retardation time = ;
- is the Upper convected time derivative of stress tensor:
- ;
- is the fluid velocity;
- is the total viscosity composed of solvent and polymer components, ;
- is the deformation rate tensor or rate of strain tensor, .
The model can also be written split into polymeric (viscoelastic) part separately from the solvent part: .
where
Whilst the model gives good approximations of viscoelastic fluids in shear flow, it has an unphysical singularity in extensional flow, where the dumbbells are infinitely stretched; If the solvent viscosity is zero then the Oldroyd-B becomes the Upper Convected Maxwell model.
References
- Oldroyd, James (Feb 1950). "On the Formulation of Rheological Equations of State". Proceedings of the Royal Society of London. Series A, Mathematical and Physical Sciences 200 (1063): 523–541.
- Owens, R. G.,Phillips, T. N. (2002). Computational Rheology. Imperial College Press. ISBN 978-1-86094-186-3.
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